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ElectricalMachine
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The force per unit length existing between two infinite parallel conductors is given by ___________

A

╬╝0I1I22╧Аd\frac{\mu_0 I_1 I_2}{2\pi d}2╧Аd╬╝0тАЛI1тАЛI2тАЛтАЛ

B

╬╝0I1I22d\frac{\mu_0 I_1 I_2}{2d}2d╬╝0тАЛI1тАЛI2тАЛтАЛ

C

╬╝0I1I2d\frac{\mu_0 I_1 I_2}{d}d╬╝0тАЛI1тАЛI2тАЛтАЛ

D

╬╝0I1d\frac{\mu_0 I_1}{d}d╬╝0тАЛI1тАЛтАЛ

Correct Answer

тЪЩя╕П TE тАв Technical Concept & PrincipleElectricalMachine
Option A

╬╝0I1I22╧Аd\frac{\mu_0 I_1 I_2}{2\pi d}2╧Аd╬╝0тАЛI1тАЛI2тАЛтАЛ

Quick Summary:

The force per unit length existing between two parallel conductors carrying currents I1I_1I1тАЛ and I2I_2I2тАЛ separated by a distance ddd in free space is given by F/L=╬╝0I1I22╧АdF/L = \frac{\mu_0 I_1 I_2}{2\pi d}F/L=2╧Аd╬╝0тАЛI1тАЛI2тАЛтАЛ. This fundamental relationship follows from Ampere's Law and the Lorentz force principle, where the magnetic field produced by one conductor exerts a force on the current-carrying second conductor.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

The force per unit length existing between two parallel conductors carrying currents I1I_1I1тАЛ and I2I_2I2тАЛ separated by a distance ddd in free space is given by F/L=╬╝0I1I22╧АdF/L = \frac{\mu_0 I_1 I_2}{2\pi d}F/L=2╧Аd╬╝0тАЛI1тАЛI2тАЛтАЛ. This fundamental relationship follows from Ampere's Law and the Lorentz force principle, where the magnetic field produced by one conductor exerts a force on the current-carrying second conductor.

ЁЯФв Key Formulas

F/L=╬╝0I1I22╧АdF/L = \frac{\mu_0 I_1 I_2}{2\pi d}F/L=2╧Аd╬╝0тАЛI1тАЛI2тАЛтАЛ тАФ Force per unit length between two long parallel conductors

B=╬╝0I2╧АdB = \frac{\mu_0 I}{2\pi d}B=2╧Аd╬╝0тАЛIтАЛ тАФ Magnetic flux density around a long straight current-carrying wire

тЪЩя╕П Working Principle

A current I1I_1I1тАЛ flowing through an infinitely long conductor produces a magnetic flux density B1=╬╝0I12╧АdB_1 = \frac{\mu_0 I_1}{2\pi d}B1тАЛ=2╧Аd╬╝0тАЛI1тАЛтАЛ at a perpendicular distance ddd. When a second conductor carrying current I2I_2I2тАЛ is placed in this magnetic field, it experiences a magnetic force per unit length given by F/L=B1I2=╬╝0I1I22╧АdF/L = B_1 I_2 = \frac{\mu_0 I_1 I_2}{2\pi d}F/L=B1тАЛI2тАЛ=2╧Аd╬╝0тАЛI1тАЛI2тАЛтАЛ. If currents flow in the same direction, the force is attractive; if in opposite directions, it is repulsive.

ЁЯУМ Key Points
  • тЦ╕

    Parallel currents in the same direction attract each other.

  • тЦ╕

    Antiparallel (opposite direction) currents repel each other.

  • тЦ╕

    This formula is used to define the standard SI unit of current, the Ampere.

  • тЦ╕

    The force is directly proportional to the product of currents (I1I2I_1 I_2I1тАЛI2тАЛ) and inversely proportional to distance (ddd).

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Definition of the standard SI unit of current (Ampere).

  • тЦ╕

    Calculating electrodynamic forces on busbars in high-voltage switchgear during short-circuit conditions.

ЁЯУД Additional Information
  • тЦ╕

    Option B lacks the ╧А\pi╧А term in the denominator, which is required due to the cylindrical symmetry of the magnetic field.

  • тЦ╕

    Option C lacks both the constant 2 and ╧А\pi╧А in the denominator.

  • тЦ╕

    Option D represents a expression missing the second current I2I_2I2тАЛ and required constants.

ЁЯУК Diagram / Illustration
Force Per Unit Length Between Parallel ConductorsF / L =┬╡тВА IтВБ IтВВ2 ╧А dWhere ┬╡тВА = 4╧А ├Ч 10тБ╗тБ╖ H/m (Permeability of free space)
тЬЕ

A is correct тАФ The magnetic force per unit length between two infinite parallel current-carrying conductors is ╬╝0I1I22╧Аd\frac{\mu_0 I_1 I_2}{2\pi d}2╧Аd╬╝0тАЛI1тАЛI2тАЛтАЛ.

Core Concepts Used
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Ampere's Law Lorentz Force Principle Magnetic Field of Long Conductors
ЁЯТб EXAM TIP

Remember that parallel conductors with currents in the SAME direction ATTRACT, which is opposite to electrostatic charges where LIKE charges REPEL.

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